Optical information recording method and apparatus

ABSTRACT

An optical information recording method and apparatus which records information on a recording medium by irradiating the recording medium with an irradiation light of a recording power to form a recorded-mark on the recording medium such that reflection coefficient from an area of the recorded-mark is different than a reflection coefficient from an area of the recording medium where the recorded-mark is not formed by a changing power of the irradiation light. Information is recorded by modulating the irradiation light according to the information for recording, forming a recorded-mark on the recording medium by changing the power of the irradiation light between a recording power and a non-recording power, receiving reflection light of the irradiation light reflected by the recording medium and producing a corresponding light signal, determining a state of the recorded-mark based upon the light signal produced during a predetermined period of time immediately after the irradiation light changes from the recording power to the non-recording power, and controlling the recording power of the irradiation light according to the state of the recorded-mark.

CROSS REFERENCE TO RELATED APPLICATIONS

This application claims priority under 35 USC §119 to Japanese patentapplication No.10-189190 filed Jul. 3, 1998, the entire contents ofwhich is incorporated herein by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical information recording methodand an apparatus, and more particularly to an optical informationrecording method and an apparatus provided with an improvedmark-recording operation.

2. Discussion of the Background

In recent years, optical information recording apparatuses, such as acompact disk-recordable (CD-R) drive, have become commerciallypractical, and a study toward further increasing a storage capacity anda recording speed of the apparatuses is being continued. As recordableoptical disk media, for example, a write-once optical disk medium usingcoloring agent compounds, a magneto-optical disk medium, and arewritable optical disk medium using phase-change materials, are known.

In a general optical disk recording apparatus, laser light, which isemitted by a laser diode and pulse-modulated according to recordinginformation, irradiates a recording medium, changes the reflectioncoefficient of the recording medium, and thereby forms a recorded-mark.The laser light power affects the quality or the state of therecorded-mark, i.e., if the quality of the recorded-mark does notsatisfy the specification of a recording format, a data error occurs.Various states of the recorded-mark, for example, a horizontal shape, across-sectional radius of the hollow of the mark, the surfaceunevenness, the outline shape, the color, unevenness of the color, andso forth, are known. Therefore, hitherto, before starting an ordinaryinformation recording operation, in order to determine a properrecording power suitable for the characteristics of a recording medium,test writing is carried out on a predetermined area of the recordingmedium while changing the recording power. The recording power that hasrecorded a signal, which is reproduced with the best symmetry, is chosenas an optimum recording power. The optimum recording power is maintainedduring ordinary information recording on a recording medium. This methodis known as an “optimum power control” (OPC) method.

However, even when the optimum recording power, which is determined bythe above-described test writing, is maintained during the ordinaryinformation recording, other factors can disturb the accomplishment ofan optimum recording. For example, the optimum recording power forrecording depends upon the sensitivity of the recording medium, andtherefore the optimum recording power changes according to variations inthe sensitivity of the recording medium. Further, the optimum recordingpower changes according to a tilt of the recording medium relative tothe laser light. In addition, even if a drive current of the laser diodeis kept constant to keep the optimum output power for optimum recording,the actual output power of the laser diode may change due to, forexample, an environmental temperature change, causing a deviation of theoutput power from the optimum output power for the optimum recording. Inother words, even when a recording operation on a medium is performedusing the conventional OPC method, an optimum recording might not bealways possible throughout the whole area of the recording medium.

To solve these problems, for example, Japanese Patent PublicationNo.60696/1982 proposes to detect a change in reflected light of therecording light coming from the disk during an ordinary informationrecording operation. The output power of a light source is controlled inaccordance with the result of the detection. According to thispublication, while information is being recorded, the state of arecorded-mark is obtained at the same time based upon the result ofdetecting a change in reflected light from the disk, and therebyfluctuation of the recording power from an optimum recording power isdetected. Such fluctuation may have been caused by variations in theoutput power of the light source in the recording operation, a tilt ofthe disk relative to the laser light, or variations in the sensitivityof the disk. The output power of the light source is controlled so thatthe fluctuation from the optimum irradiation power is compensated. Morespecifically, in a test writing operation, each recording power and aresulting detected signal indicating a change in the reflected light arestored in a corresponding manner, and in a normal writing, the laserdiode is controlled so as to output the optimum output according to thestored information. A similar method, known as a “running-optimum powercontrol” (R-OPC) method, is in use in some CD-R drive apparatuses.

The above method, i.e., controlling the output of a light sourceaccording to the result of detecting a change in reflected light from arecorded-mark, has however problems such that the reflected light doesnot change according to the recorded mark or such that the change in thereflected light can not be accurately detected under certain recordingconditions or in a certain recording medium.

A reflection coefficient of a recorded area of a recording medium isdifferent from that of the non-recorded area of a recording medium.Reflected light power is expressed as the product of irradiation lightpower and a reflection coefficient of a part of the recording mediumcovered by an irradiation light spot. During a recording operation, theirradiation light spot moves relative to the recording medium at aconstant velocity on a recording track of the medium. Therefore, in therecording operation, the irradiation light spot always covers both arecorded portion, i.e., an area where a mark is formed, and anon-recorded portion of the recording medium in a certain ratio.Accordingly, the reflection coefficient of the area covered with theirradiation light spot can be determined as an average of those of therecorded portion and the not-recorded portion of the area of a recordingmedium covered by the irradiation light spot. However, in the recordingprocess, the ratio of a recorded portion and a not-recorded portion ofthe area covered by the irradiation light spot dynamically changes forvarious reasons. For example, variation in the sensitivity of therecording medium changes the speed of forming the recorded mark.Accordingly, the result of detecting the change of the reflected lightis apt to be influenced by any deviations in the sensitivity of therecording medium. Particularly, in a high-speed recording operation, theirradiation light spot mainly covers the non-recorded portion ratherthan a mark portion, and therefore, the reliability of detecting thechange of the reflected light is apt to be decreased. Accordingly, thedifficulty in accurately detecting the change of the reflected lightincreases in proportion to the recording velocity.

Further, when a multiple-pulse method, which is suited and is oftenutilized for a large capacity recording, is used as a method of forminga mark, a pulse train of a recording heating-pulse and a breakingbottom-power pulse is repeated in a short time. That is, the pulse isturned to the breaking pulse or the bottom-power pulse in a short timeafter reflected light of a recording pulse or a heating-pulse isreceived, and thereby reflected light is suddenly decreased. Therefore,a high speed detecting device and a circuit are required for anappropriate detection of the changes in the reflected light.

SUMMARY OF THE INVENTION

Accordingly, one object of this invention is to provide a novel opticalinformation recording method and an apparatus that are capable of acontrolled forming of an appropriate recording-mark by compensating fordeviations from optimum recording caused by variation in irradiationpower from the light source, a tilt of a recording medium, and/orvariation of the recording medium regardless of a recording medium, arecording method, or a range of recording velocity. The presentinvention compensates for these deviations by detecting the state of amark being formed.

One embodiment of the optical information recording method includessteps of modulating the irradiation light according to the informationfor recording, such steps comprising forming a recorded-mark on therecording medium by changing power of the irradiation light between arecording power and a not-recording power, receiving reflection lightfrom the irradiation light reflected by the recording medium, convertingthe received reflection light into a received light signal, determininga state of the recorded-mark based upon the received light signal of thereflection light which is received during a predetermined period of timeimmediately after the irradiation power changes to the non-recordingpower, and controlling the recording power of the irradiation lightaccording to the state of the recorded-mark.

BRIEF DESCRIPTION OF THE DRAWINGS

A more complete appreciation of the present invention and many of theattendant advantages thereof will be readily obtained as the samebecomes better understood by reference to the following detaileddescription when considered in connection with the accompanyingdrawings, wherein:

FIG. 1 is a functional block diagram illustrating an exemplaryconstruction of an optical information recording apparatus according toan embodiment of the present invention;

FIG. 2 is a graph illustrating a relation among irradiation light, arecorded-mark shape, a reflection coefficient, and reflected lightpower;

FIG. 3 illustrates a relation between a light spot of irradiation lightand recorded-marks;

FIG. 4 is a plot illustrating a relation between recording-power andreflected light by a mark recorded on a recording medium;

FIG. 5 is a graph illustrating waveforms of reflected light signal RF ina vicinity when a laser diode switched to output a pedestal power as afunction of time for comparison to a state of a recorded-mark;

FIG. 6 is the same waveforms of FIG. 5 illustrating differences amongthe reflected light signals RF at a certain time tat from the laserdiode 1 starts outputting the pedestal power;

FIG. 7 is a magnified graph of the waveforms of FIG. 5 in a vicinity oftime elapsed ta1 from the laser diode 1 starts outputting the pedestalpower, illustrating gradient differences of reflected light signal RFdepending upon the state of a recorded-mark;

FIG. 8 is the same waveforms of FIG. 5 illustrating time differencesfrom the laser diode 1 starts outputting the pedestal power to thereflected light signal RF becomes a certain value depending upon thestate of a recorded-mark;

FIG. 9 is a flowchart illustrating the steps in a method for controllinga recording-power of the embodiment;

FIG. 10 is a flowchart of a test writing illustrating the steps in amethod to determine a control target for acquiring a desiredrecorded-mark;

FIG. 11 is a functional block diagram illustrating an opticalinformation recording apparatus according to another embodiment of thepresent invention;

FIG. 12 is a graph illustrating waveforms of reflected light signal RFof the functional block diagram of FIG. 11;

FIG. 13 is a functional block diagram illustrating an opticalinformation recording apparatus according to still another embodiment ofthe present invention;

FIG. 14 is a flowchart illustrating the steps in a method forcontrolling the recording-power of the optical information recordingapparatus of FIG. 13;

FIG. 15 is a functional block diagram illustrating an opticalinformation recording apparatus according to still another embodiment ofthe present invention;

FIG. 16 is a graph illustrating waveforms of reflected light signal RFof the optical information recording apparatus of FIG. 15;

FIG. 17 is a flowchart illustrating the steps in a method forcontrolling the recording-power of the optical information recordingapparatus of FIG. 15;

FIG. 18 is a functional block diagram illustrating an opticalinformation recording apparatus according to still another embodiment ofthe present invention;

FIG. 19 is a graph illustrating waveforms of reflected light signal RFof the optical information recording apparatus of FIG. 18 and pulsegenerated by a comparator;

FIG. 20 is a graph illustrating a relation between input and output of apulse-detecting device;

FIG. 21 is a functional block diagram illustrating an opticalinformation recording apparatus according to still another embodiment ofthe present invention;

FIG. 22 is a graph illustrating waveforms of reflected light signal RFof the optical information recording apparatus of FIG. 21 and areference value of a comparator;

FIG. 23 is a functional block diagram illustrating an opticalinformation recording apparatus according to yet another embodiment ofthe present invention;

FIG. 24A is a graph illustrating waveforms of irradiation light power ina multiple-pulse recording method;

FIG. 24B is a graph illustrating waveforms of reflected light signal RFin the multiple-pulse recording method;

FIG. 24c illustrates a recorded-mark by the multiple-pulse recordingmethod;

FIG. 25 is a flowchart illustrating the steps in a method forcontrolling the recording-power of the multiple-pulse recording method;

FIG. 26 is another flowchart illustrating the steps in a method forcontrolling the recording-power of the multiple-pulse recording method;

FIG. 27 is a graph illustrating waveform magnified of reflected lightsignal RF from a recording medium having a certain kind of heatsensitive recording layer;

FIG. 28A is a graph illustrating a waveform of irradiation light powerin a heat-mode recording with the multiple-pulse recording method;

FIG. 28B is a graph illustrating a waveform of reflected light signal RFfrom a recording medium having a certain kind of heat sensitiverecording layer with the multiple-pulse recording method; and

FIG. 28c illustrates a recorded-mark by the heat mode recording with themultiple-pulse recording method.

DESCRIPTION OF THE PREFERRED EMBODIMENT

Referring now to the drawings, wherein like reference numerals designateidentical or corresponding parts throughout the several views, and moreparticularly to FIG. 1 thereof,

FIG. 1 is a block diagram illustrating an optical information recordingapparatus 101 according to an embodiment of the present invention.Referring to FIG. 1, the optical information recording apparatus 101includes a laser diode 1, a laser diode control device 2, a recordingmedium 3, a light pickup 4, a light-receiving device 5, and a mark-statedetermining device 6. The laser diode 1 is a light source to irradiatethe recording medium 3 for recording a mark as data thereupon andreading the mark as the data therefrom. The laser diode control device 2controls the laser diode 1 to modulate the output power thereofaccording to recording data.

The light-pickup 4 includes an object lens to focus the irradiationlight PL emitted by the laser diode 1 onto the recording medium 3 and tocollect light reflected by the recording medium 3. The recording medium3 has a recording layer that is recordable by a photon-mode reaction ora heat-mode reaction by the irradiation laser diode 1. The lightreceiving device 5 includes a photoelectric converter that receivesreflected light Pd of the irradiation light PL, which is reflected bythe recording medium 3, through the light-pickup 4, and then convertsthe received light into a received light signal RF. The mark-statedetermining device 6 determines a state of a recorded-mark based uponthe received light signal RF after the output power of the laser diode 1transits to a “pedestal power” Pp from a recording-power Pw before thenext mark recording operation. Hereinafter, the term “pedestal power” isreferred to as output power of the laser diode 1 that does not form anyrecorded-marks. The “pedestal power” Pp can be equal to bottom-power ina multiple-pulse recording method. The “pedestal power” Pp can be equalto reading-power, or can be smaller than the reading-power but greaterthan zero, or greater than the reading-power but smaller than therecording-power Pw. The term “recording-power” is referred to as outputpower of the laser diode 1 that can form recorded-marks.

The mark-state determining device 6 generates a mark-state signal Vdtcaccording to the state of a recorded-mark, and then sends the mark-statesignal Vdtc to the laser diode control device 2 as a feedback signal forthe recording-power Pw. The laser diode control device 2 determines adeviation of the recording-power Pw from an optimum recording-power forthe moment of recording the mark producing the mark-state signal Vdtc,and then controls the output power of the laser diode 1 such that therecording-power Pw becomes the optimum recording-power.

The optical information recording apparatus 101 further includes a servocontrol device (not shown) that controls the light-pickup 4 to place alight spot LSP irradiating the recording medium 3 at any given placesthereof, and others.

FIG. 2 illustrates a relation among irradiation light, a recorded-markshape, a reflection coefficient, and reflected light power. In FIG. 2,“IRRADIATION LIGHT PL” indicates a waveform of a irradiation light ofthe laser diode 1, “MARK SHAPE” indicates a shape of a recorded-mark Mon the recording medium 3 formed by the irradiation light PL,“REFLECTION COEFFICIENT” indicates a waveform of a reflectioncoefficient of the recording medium 3 having the recorded-mark M, and“REFLECTED LIGHT Pd” indicates a waveform of reflected light reflectedby the recording medium 3. In the illustration of “IRRADIATION LIGHTPL”, Pw indicates the “recording-power” and Pp indicates the “pedestalpower”. Time t0 and time t10 indicate a start and an end of therecording-power Pw respectively, and time t11 indicates a start of thepedestal power Pp. The time t10 and the time t11 can be practically thesame time. The pedestal power Pp is smaller than the recording-power Pwso as not to form any recording marks and can be for example,substantially the same as the reading-power.

Under these conditions, the irradiation light PL of the laser diode 1irradiates the recording medium 3 through the light pickup 4. Therecording medium 3 is kept rotating such that a light spot LSP, which isemitted by the laser diode 1 and which is focused by the light pickup 4,moves relative to the medium 3 at a substantially constant linearvelocity at all irradiated places. The recording medium 3 can be rotatedin a constant angular velocity, which is called as a “CAV method”;however, even in the CAV method, a linear velocity at a certain radiallocation is still constant. Therefore, the light spot LSP moves relativeto the medium 3 at a constant velocity on a recording track of therecording medium 3.

Accordingly, the light spot LSP with the recording-power Pw forms arecorded-mark M as shown as “mark M” in FIG. 2. That is, when arecorded-mark M is formed by irradiation heat of the laser diode 1,because of a photochemical reaction time and/or a heat capacity of therecording medium 3, the “mark M” will not be formed instantly when theirradiation with the recording-power Pw starts. In other words, theformation of the “mark M” does not start at the time t0 when therecording-power Pw starts to irradiate but starts a certain time afterthe time t0 as shown in FIG. 2. The end of the “mark M” can be delayedfrom the end of the irradiation of the light spot LSP with therecording-power Pw due to the photochemical reaction time and/or theheat capacity of the recording medium 3 as well. The width of the “markM” perpendicular to the locus is smaller than the diameter of the lightspot LSP in the embodiment. On the other hand, an area where therecorded-mark M is not formed is referred to as “space”.

Referring to “REFLECTION COEFFICIENT” in FIG. 2, RCs and RCm indicatereflection coefficients of the “space” and “mark” respectively. Areflection coefficient of the “mark” is smaller than that of the “space”in the embodiment. A reflection coefficient in the boundary between the“space” and the “mark” can be between of RCm and RCs. Referring toREFLECTED LIGHT Pd in FIG. 2, the reflected light power Pd isapproximated as the product of the irradiation light PL of the laserdiode 1 and the reflection coefficient of a part of the recording medium3, which is covered by the light spot LSP.

In FIG. 2, before reaching the time t0, the irradiation light PL has thepower Pp, and the light spot LSP of the irradiation light PL covers only“space”. Consequently, the product of the irradiation light PL and thereflection coefficient, i.e., the reflected light power Pd, is Pp×Rcs.At the time t0, the irradiation light PL is changed to Pw, however, thelight spot LSP of the irradiation light PL covers only the “space” area,because the mark has not yet formed at the moment, and consequently, thereflected light power Pd becomes Pw×Rcs. Immediateluy after the time t0,the “mark M” is formed, and the light spot LSP of the irradiation lightPL cover both “mark M” and “”. And consequently, the reflected lightpower Pd becomes smaller than Pw×RCs and is gradually decreased. At thetime t10, the irradiation light PL is not yet changed to Pp and thelight spot LSP of the irradiation light PL covers both “mark M” area(referred to as “Am”) and “space” area (referred to as “As”), andconsequently, the reflected light power Pd becomesPw×(RCm×Am+RCs×As)/(Am+As). At the time t11, when the recording power Pwchanges to the pedestal power Pp, the light spot LSP of the irradiationlight PL covers substantially the same areas at the time t10;consequently, the reflected light power Pd isPp×(RCm×Am+RCs×As)/(Am+As). After the time t11, the reflected lightpower Pd gradually approaches to Pp×RCs.

FIG. 3 illustrates a relation between a light spot size of irradiationlight and a recorded-mark at the vicinity of the trailing end of arecorded mark at the time t10 or t11 in FIG. 2. In FIG. 3, a doted line“A” illustrates a mark formed with recording-power Pwa that is smallerthan an optimum recording-power. A line “B” illustrates a mark formedwith the optimum recording-power Pwb. A doted line “C” illustrates amark formed with recording-power Pwc that is larger than the optimumrecording-power. A deviation from the optimum recording-mark is causedby not only the deviation of the recording-power from the optimumrecording-power, but also by other reasons, such as, for example,sensitivity variation of the recording medium 3, a tilt of the recordingmedium 3 relative to the laser light, a defocused light spot of theirradiation light PL, and so on. The tilt of the recording medium 3 andthe defocused light spot deform the light spot LSP, and thereby theresulting recorded-mark becomes different from the one resulting from anideal light spot shape. The deviation of the recording-power from theoptimum recording-power Pwb can be caused, for example, by a settingerror for a control target or an output power drift of the laser diode 1due to a temperature change.

FIG. 4 is a plot illustrating a relation between recording-power andpower of light reflected by a mark recorded on a recording medium. Thereflection coefficient of the recorded-mark M is smaller than that ofthe “space” in the embodiment. And when the light spot LSP covers both apart of the “mark M” and the “space”, the power of the light reflectedby an area that is irradiated by the light spot LSP is approximatelyinversely proportional to that of the light reflected by the part of therecorded mark M. Accordingly, at time t11 (FIG. 2), the reflected lightpower Pd of the light spot LSP is approximately inversely proportionalto that of the light reflected by the part of the recorded-mark M, i.e.,the reflected light Pd is approximately inversely proportional to therecording power Pw as shown in FIG. 4. In FIG. 4, when recording poweris Pwa, the light forms a “mark M” shown as “A” in FIG. 3, and therecorded mark reflects light with intensity Ra at time t11. Likewise,when recording power is Pwb, the recorded mark reflects light withintensity Rb. And when recording power is Pwc, the recorded markreflects light with intensity Rc.

FIG. 5 is a graph illustrating waveforms of a reflected light signal RF,which is converted from the reflected light Pd by the light-receivingdevice 5, in the vicinity where the laser diode 1 switches to output thepedestal power Pp. In FIG. 5, a waveform “a” indicates a reflected lightsignal RF by a mark M formed like “A” in FIG. 3 with recording lightPwa. Likewise, the waveform “b” indicates a reflected light signal RF bya mark M formed like “B” in FIG. 3 with the recording light Pwb, and thewaveform “c” indicates a reflected light signal RF by a mark M formedlike “C” in FIG. 3 with the recording light Pwc. As these waveformsshow, the waveform of a reflected light signal RF changes according tothe shape of “the mark M”. Therefore, the state of a recorded mark canbe determined based upon the detected result of the reflected lightsignal RF.

The reflected light signal RF is proportional to the product of theirradiation light PL and an area of “space”. The mark area covered bythe light spot LSP gradually approaches zero, or the space area coveredby the light spot LSP gradually approaches whole the light spot LSP.Consequently, the waveforms of “a, “b”, and “c” converge at a constantvalue Vs, which is approximately the same as the product of theirradiation light PL of the laser diode 1 and the reflection coefficientof the recording medium 3.

FIG. 6 is a graph of waveforms of FIG. 5 illustrating differences amongthe reflected light signals RF at time after ta1 from t11. In FIG. 6,the laser diode 1 starts outputting the pedestal power Pd at time t11.“t12” represents a time whereta1 is elapsed from t11. “Vsat” representsa reflected light signal RF at t12 when a mark M is formed like “A”shown in FIG. 3. Likewise, “Vsbt” represents a reflected light signal RFat t12 when a mark M is formed like “B” ; “Vsct” represents a reflectedlight signal RF at tl2 when a mark M is formed like “C”. Thus, the stateof a recorded-mark can also be detected by using differences in thereflected light signal RF at a certain time after the laser diode 1starts outputting the pedestal power Pp.

FIG. 7 is a magnified graph of the waveforms of FIG. 5, in the vicinityof time t12 whereta1 is elapsed from t11, illustrating a gradient ofeach reflected light signal RF. “t12” indicates a time whereta1 iselapsed from t11, “dt” indicates a short time, “dla”, “dlb”, and “dlc”indicate a change in each of the reflected light signals RF. Thereby,each dla/dt, dlb/dt, and dlc/dt represents a gradient of the graphs att12. The gradient depends upon the state of a recorded mark. In thisembodiment, the gradient dla/dt is the smallest and the gradient dlc/dtis the greatest among the three. Accordingly, the state of a recordedmark can also be determined according to the gradients. The timederivative of the waveform of a reflected light signal RF at t12 can beused, instead of the gradient, as well, for determining the state of arecorded-mark.

FIG. 8 is a graph of the waveforms of FIG. 5, illustrating timedifferences from a time when the laser diode 1 starts outputting thepedestal power Pp to a time when the reflected light signal RF becomes acertain value for each of the recorded mark A, B, and C of FIG. 3.“Vref” indicates a reference value or a threshold value of the reflectedlight signal RF. ta, tb, and tc respectively indicate a periods of timefrom t11 to the time when the reflected light signal RF reaches thevalue Vr. The period depends upon the state of a recorded-mark. Forexample, the period is approximately proportional to the size of arecorded-mark M. In this embodiment, ta is the smallest, and tc is thegreatest among the three. Accordingly, the state of a recorded-mark canalso be determined according to these periods.

FIG. 9 is a flowchart illustrating exemplary steps of an operation forcontrolling the recording-power according to an embodiment of thepresent invention. The control steps are executed for each operation offorming a recorded-mark or at a predetermined interval of the operationof forming a recorded-mark. Reference symbol Vtgt represents a controltarget for the mark-state signal Vdtc. The step S12 and step S13 arereferred to as S12-13. In the step S12, the laser diode 1 startsirradiation with recording-power Pw to the recording medium 3 at time t0of FIG. 2, and formation of a recorded-mark M is started. During thestep S12-13, the laser diode control device 2 controls the laser diode 1to output a proper irradiation light to form a recorded-mark such that amark state signal Vdtc obtained from a reflected light from therecording medium coincides to a control target Vtgt, utilizing apreviously obtained mark-state signal Vdtc. In other words, when themark-state signal Vdtc, which has been obtained with a mark M formed ina previous recording operation, is too large or too small relative tothe control target Vtgt, the laser diode control device 2 controls thelaser diode 1 to emit proper irradiation light according to thedifference between the control target Vtgt and the mark-state signalVdtc.

In the step S14, at time t10 of FIG. 2, the laser diode control device 2switches the irradiation power of the laser diode 1 from therecording-power Pw to the pedestal power Pp. At this moment, theformation of a recorded-mark M is completed, and the recorded-mark M isformed as “Mark M” in FIG. 2.

Step Sop1 is a timer and is optional. When the Step Sop1 is executed, adetecting operation in step S15 is executed time ta1 after time t10.

In step S15, if the step Sop1 is executed at time t12 of FIG. 6 or FIG.7, or, at time t11 of FIG. 2 which is substantially the same as timet10, the light-receiving device 5 receives reflected light Pd from therecording medium 3 and converts the received light Pd into a receivedlight signal RF. When the step Sop1 was executed, the received lightsignal RF such as “Vsb” of FIG. 5 is obtained. When the step Sop1 wasnot executed, the received light signal RF such as “Vsbt” of FIG. 6 isobtained.

In step S16, the mark-state determining device 6 determines the state ofthe recorded-mark according to the received light signal RF andgenerates a mark-state signal Vdtc as a feedback signal for a nextrecording mark formation. The mark-state determining device 6 sends themark-state signal Vdtc as the state of the recorded-mark to the laserdiode control device 2 for the next recording mark formation. Themark-state determining device 6 can use, in addition to the receivedlight signal RF, various information to determine the state of arecorded-mark. For example, a recording velocity, data of the materialof the recording medium 3, such as the sensitivity data, the standardreflection coefficients of the “mark” and the “space”, temperature inthe recording apparatus 101, and so forth, can be used. In step S18, ifany recording data is left, the operation returns to step S12.

FIG. 10 is a flowchart of an exemplary test writing operation,illustrating steps for determining a control target Vtgt. The testwriting can be executed, for example, when the optical informationrecording apparatus 101 is turned-on or connected to a host computer,when the recording apparatus 101 receives a command from the computer,when a new recording media disk is inserted to the recording apparatus101, when temperature inside the recording apparatus 101 is changed. Ortest writing can be executed at a predetermined interval, and so forth.The test writing can be done using a predetermined area of the recordingmedia desk 3, such as, a part of the outer or inner regions thereof.

In step ST12, the laser diode 1 starts irradiation with initialrecording-power Pw to the recording medium 3 at time t0 of FIG. 2. Instep ST13, at time t10 of FIG. 2, the laser diode control device 2switches the irradiation power of the laser diode 1 to the pedestalpower Pp from the recording-power Pw. In step ST14, at time t11 of FIG.2, the light-receiving device 5 receives reflected light Pd from therecording medium 3 and converts the received light Pd into a receivedlight signal RF. Then, a pair of the received light signal RF data andthe recording-power Pw data is stored in a memory MEM, provided, forexample, inside the mark-state determining device 6. The above operationof obtaining the received light signal RF and storing the pair of thereceived light signal RF data and the recording-power Pw data can beexecuted at time afterta1 from t11, shown as t12, in FIG. 6 or FIG. 7.

A path from the step ST12 through the step ST15 is repeated apredetermined number of times N with changing the recording-power Pw. Inthe step ST15, whether the predetermined number of times N of the pathis completed is judged. If the predetermined number of times N of thepath is not completed, the operation goes to step ST16. In step ST16,the recording-power Pw is incremented by a predetermined value. If thepredetermined number N of times of forming and detecting the marks iscompleted, N pair of the received light signal RF data and therecording-power Pw data are stored in the memory MEM.

In step ST17, those pairs of the data are evaluated from the viewpointof, for example, deviations of length of both a recorded short mark anda recorded long mark from specified length according to a specificrecording format, and then a pair of the received light signal RF dataand the recording-power Pw data, which recorded the recorded-marks withminimum deviation from the specification, is chosen as the controltarget “Vtgt”.

FIG. 11 is a functional block diagram illustrating an opticalinformation recording apparatus 102 according to another embodiment ofthe present invention. In FIG. 11, functional blocks that aresubstantially the same as those in FIG. 1 are denoted by the samereference numerals. The optical information recording apparatus 102includes a system control device 90. The system control device 90 canbe, for example, a micro computer system having a CPU, a RAM, a ROM, anon-volatile memory, an input output device, a host computer interface90A, an external bus 90B, and so forth.

The mark-state determining device 6 includes a bottom-hold device 10 anda sampling device 11. The bottom-hold device (i.e. a minimum valuestoring device) 10 is a circuit to detect and hold a bottom or a minimumvalue of received light signals RF that are output from thelight-receiving device 5. The sampling device samples or retrieves thebottom value of received light signal RF held by the bottom-hold device10 and converts the sampled signal into digital data by a built-inanalog to digital converter.

FIG. 12 is a graph illustrating waveforms of reflected light signal RFoutput from the light receiving device 5 and input to the mark-statedetermining device 6 in the functional block diagram of FIG. 11.Referring FIG. 12, “a”, “b”, and “c” are waveforms of reflected lightsignals RF, each representing a state of a recorded-mark. Thebottom-hold device 10 becomes ready to hold a bottom value of receivedlight signal RF before the received light signal RF is output, i.e.,before the time t11. And thereby at the time t11, the bottom-hold device10 holds the signal RF and outputs the held signal, such as the oneshown as Vsa, Vsb, or Vsc, depending upon the state of a mark, such as“A”, “B”, or “C” of FIG. 3. At time after TS1 from t11, the samplingdevice 11 retrieves the held bottom value of the received light signalRF and converts the held signal into digital data Vdtc, and sends thedata Vdtc as feedback data of the state of a recorded-mark to the laserdiode control device 2.

The laser diode control device 2 controls the laser diode 1 according tothe received mark-state signal Vdtc to emit proper irradiation light toform a recorded-mark such that a mark-state signal Vdtc of the nextrecording mark coincide with the control target Vtgt. The mark-statedetermining device 6 can also use another information to determine thestate of a recorded-mark, such as, recording velocity data and materialcharacteristics data of the recording medium 3, which are stored in thesystem control device 90.

FIG. 13 is a functional block diagram illustrating an opticalinformation recording apparatus 103 according to still anotherembodiment of the present invention. In this embodiment, the recordingpower is controlled in substantially the same manner as in theembodiment shown in FIG. 11. However, the pedestal power Pp iscontrolled by an automatic power control (APC) system for compensating,for example, a temperature drift of the laser diode 1. The APC systemstabilizes the pedestal power Pp of the laser diode 1, and as a result,detection of a light reflected by a recorded-mark M and the generationof a mark-state signal Vdtc are not affected by the temperature drift ofthe laser diode 1. Consequently, controlling accuracy of the recordingpower Pw is further improved. The APC system monitors only a part ofradiation of the laser diode 1. Further, the APC system only controlsthe pedestal power Pp thereof. Therefore, the APC system requiresneither a high speed nor a high drive current as the recording power Pw.Consequently, the APC system in the embodiment can be constructed with areasonably low fabrication cost.

Referring to FIG. 13, the optical information recording apparatus 103includes, in addition to the devices of FIG. 11, a photodiode 12 as alight detector, a sample and hold device 13, an automatic power control(APC) device 14, and a selector 50. The photodiode 12 directly detects apart of light emitted from the laser diode 1 and sends detected signalinto the sample and hold device 13. The sample and hold device 13samples and holds the output from the photodiode 12 at a timing of asampling signal S3, and sends the held signal into the APC device 14.The sampling signal S3 is generated by the system control device 90 attime t11 or after a predetermined time after t11 of FIG. 2. And thereby,the sample and hold device 13 samples and holds the input from thephotodiode 12 while the laser diode 1 is emitting the pedestal power Ppradiation. The APC device 14 controls the laser diode 1 to emit apredetermined radiation level of the pedestal power Pp according to thesampled data sent from the sample and hold device 13.

FIG. 14 is a flowchart illustrating an exemplary operation forcontrolling the recording-power of the optical information recordingapparatus 103. In FIG. 14, the operations are substantially the same asthose of FIG. 9 except steps S14 a, S15 a, S19, and S20. In the step S14a, at time t10 of FIG. 2, the selector 50 is switched to input a signalfrom the APC device 14. Thereby, the irradiation power of the laserdiode 1 is switched to a predetermined pedestal power Pp controlled bythe APC device 14 from the recording-power Pw controlled by the laserdiode control device 2. At this moment, forming of a recorded-mark M iscompleted and the recorded-mark M is formed as shown as “Mark M” in FIG.2. In the step S19, the sample and hold device 13 samples and holds theinput signal from the photodiode 12 and sends the signal into the APCdevice 14. In the step S20, the APC device 14 controls the laser diode 1to emit the predetermined radiation level of the pedestal power Ppaccording to the sampled signal.

In step S15 a, after the above operation of step S20, thelight-receiving device 5 receives reflected light Pd from the recordingmedium 3 and converts the received light Pd into a received light signalRF. After that, the selector 50 is again switched to input a signal fromthe laser diode control device 2.

FIG. 15 is a functional block diagram illustrating an opticalinformation recording apparatus 104 according to still anotherembodiment of the present invention. FIG. 16 is a graph illustratingwaveforms of reflected light signal RF and sampling timings in theoptical information recording apparatus 104 of FIG. 15. FIG. 17 is aflowchart illustrating an exemplary operation for controlling therecording-power of the optical information recording apparatus 104.Referring to FIG. 15, the mark-state determining device 6 includes abottom-hold device 10, a first sampling device 11, a second samplingdevice 15, and a divider 16. The bottom hold device 10 and the firstsampling device 11 retrieve the bottom value Vsb of the reflected lightsignal RF, which will fluctuate with the intensity of the pedestal powerPp, a state of a recorded-mark M and the reflection coefficient RCs of“space” of the recording medium 3. The second sampling device 15includes an analog to digital converter and samples and holds thesaturated reflected light signal RF, which also will fluctuate with theintensity of the pedestal power Pp or by the reflection coefficient RCsof “space” of the recording medium 3.

Referring to FIG. 16, a line “b” illustrates a waveform of a reflectedlight signal RF reflected from an optimum mark with irradiation ofpedestal power Pp. A line “bs” illustrates a waveform of a reflectedlight signal RF reflected from the optimum mark with irradiation ofpedestal power Pds, which is greater than Pd. Lines “as” and “cs”illustrate waveforms of reflected light signals RF, which are reflectedby a mark deviated from the optimum mark, such as “a” or “c” of FIG. 3,with irradiation of pedestal power Pds. “Vs” is the value of reflectedlight signal RF when the light spot LSP of the laser light is reflectedfrom “space” area. The value of “Vs” can be changed, for example, to“VSS” as shown in FIG. 16, due to a change of the pedestal power Pds anda change of the reflection coefficient RCs of “space” of the recordingmedium 3.

In FIG. 17, the operations of steps S12, S13, S14, and S18 aresubstantially the same as those of FIG. 9. After the step S14, thebottom value Vsb of the reflected light signal RF is held by the bottomhold device 10. In step S25, at a time TS1 after t11, the first samplingdevice 11 retrieves the bottom value Vsb. Then, the first samplingdevice 11 converts the retrieved value into digital data and sends thedata to the divider 16. In step S26, at a time TS2 after t11, the secondsampling device 15 samples and holds the saturated value Vs, which isoutput when the light spot LSP of the laser light covers only “space”area. Then, the second sampling device 15 converts the retrieved valueinto digital data and sends the data into the divider 16. In step S27,the divider 16 divides the first-sampled data Vsb by the second-sampleddata Vb, and then the quotient Vsb/Vb is sent to the laser controldevice 2 preparing for the operation of steps S12 and S13 of a next markforming operation.

As described above, the mark-state signal Vdtc is obtained as Vsb/Vb,i.e., the mark-state signal Vdtc is normalized data. Accordingly, evenif the pedestal power Pds or the reflection coefficient RCs of “space”of the recording medium 3 fluctuate, the mark-state signal Vdtc, i.e.,Vsb/Vs can determine in a precise manner the fluctuation according tothe state of a recorded-mark M formed in the steps S12 through S14.

In addition, the first sampling device 11 and the second sampling device15 can be integrated into a single device so as to be used in amultiplexed manner. When two marks are apart in a short space, andthereby an enough time for sampling the Vs at TS2 is not available, thesampling can be skipped and postponed until two marks having a longerspace appear. The length of a space between two marks depends on theinformation being recorded.

FIG. 18 is a functional block diagram illustrating an opticalinformation recording apparatus according to still another embodiment ofthe present invention, in which the mark-state determining device 6includes a comparator 17 and a pulse-width detecting device 18. Thecomparator 17 compares the reflected light signal RF and a referencevalue Vref as a threshold value, and generates a pulse according to theresult of the comparison the detection. The pulse-width detecting device18 detects the pulse generated by the comparator 17.

FIG. 19 is a graph illustrating waveforms of the reflected light signalRF of the optical information recording apparatus of FIG. 18 and pulsegenerated by the comparator 17. Referring to FIG. 19, waveforms COa,Cob, and COc are the output of the comparator 17. The reference valueVref is set below Vs, which is the value of reflected light signal RFwhen the light spot LSP of the laser light is reflected from “space”area. The comparator 17 outputs “high” at time t11, and turns the outputto “low” when the reflected light signal RF reaches the reference valueVref. Thereby, when the reflected light signal RF is “b”, the comparator17 outputs a pulse COb having width Wb. Likewise, when the reflectedlight signal RF is “a”, the comparator 17 outputs COa having width Wa,and when the reflected light signal RF is “c”, the comparator 17 outputsCOc having width Wc. Thus, the output pulse width of the comparator 17depends upon a state of a recorded-mark M, i.e., when the recordingpower of laser diode 1 is too large, the output pulse width of thecomparator 17 becomes wider than that of an optimum power, and viceversa.

FIG. 20 is a graph illustrating a relation between input and output ofthe pulse-width detecting device 18. The pulse-width detecting device 18converts the pulse output from the comparator 17 into a value, which isapproximately proportional to the width of the pulse as shown in FIG.20. The conversion from a pulse width to a value, such as a voltage, canbe done by using a low pass filter. Then, the pulse-width detectingdevice 18 sends the converted value as a mark-state signal Vdtc to thelaser diode control device 2.

The laser diode control device 2 controls the laser diode 1, accordingto the output of pulse-width detecting device 18, so as to form arecorded-mark such that a mark-state signal Vdtc from the recorded-markcoincides the control target Vtgt. The control target Vtgt is obtainedusing the comparator 17 and the pulse-width detecting device 18 at atest writing.

FIG. 21 is a functional block diagram illustrating an opticalinformation recording apparatus 106 according to still anotherembodiment of the present invention. FIG. 22 is a graph illustratingwaveforms of reflected light signal RF of the optical informationrecording apparatus of FIG. 21. In the embodiment, a reference valueVref is a variable value that varies according to the reflected lightsignal RF from “space”. Referring to FIG. 21 and FIG. 22, the mark-statedetermining device 6 includes a sampling device 19 for sampling thereflected light signal RF and a reference signal generator 20. The Vssampling device 19 samples and holds the reflected light signal RF from“space”, i.e., “Vs” at time ts in FIG. 22. The reference signalgenerator 20 generates a reference signal Vref according to the sampledand held Vs, for example, a value Vs itself or a value with offset dvfrom Vs. Then, the. reference signal generator 20 sets the referencesignal Vref to the comparator 17. The setting of variable valuereference signal Vref can be done at a test writing, which is performed,for example, every time when a recording medium 3 is changed.

The reflected light signal RF from “space” can be affected by thepedestal level irradiation power of the laser diode 1 or the reflectioncoefficient RCs of the recording medium 3 at “space”. However, even ifVs, i.e., the reflected light signal RF from “space”, is changed as “bs”shown in FIG. 22, the reference signal Vref is also changed to Vrefs asshown in FIG. 22. Thus, the comparator 17 can compare the reflectedlight signal RF with the modified reference value Vrefs, and correctlygenerate a pulse according to the detection. Accordingly, a fluctuationof the pedestal level irradiation power of the laser diode 1 or adeviation of the reflection coefficient RCs of the recording medium 3 iscanceled, so that the recording power Pw is accurately controlled.

FIG. 23 is a functional block diagram illustrating an opticalinformation recording apparatus 107 according to still anotherembodiment of the present invention. In the embodiment, the mark-statedetermining device 6 includes a bottom-hold device 30, a sampling device31, a comparator 37, and a pulse-detecting device 38. The comparator 37compares the reflected light signal RF and a reference value Vref or athreshold value, and the comparator generates a pulse according to theresult of the comparison detection. The bottom-hold device 30 holds abottom or a minimum value of received light signals RF that is outputfrom the light-receiving device 5. The sampling device samples orretrieves the held bottom value of received light signal RF by thebottom-hold device 30 and sends the data Vdtc1 as first feedback data tothe laser diode control device 2.

The pulse-width detecting device 18 detects the pulse generated by thecomparator 37, converts the pulse output from the comparator 37 into avalue Vdtc2, which is approximately proportional to the width of thepulse, and sends the converted value Vdtc2 as second feedback data tothe laser diode control device 2.

The laser diode control device 2 controls the laser diode 1 according tothe Vdtc1 and Vdtc2 so as to form a recorded-mark such that a averagevalue of the mark-state signals Vdtc1 and Vdtc2 coincides the controltarget Vtgt.

FIG. 24A is a graph illustrating a waveform of irradiation light powerin a multiple-pulse recording method. In the FIG. 24A, “Pp” indicatespedestal power, “Pb” indicates bottom power, and “Pw” indicates arecording power. The pedestal power “Pp” can be equal to the bottompower “Pb”. “t10” represents end of a plurality of recording pulses and“t11” represents start of the pedestal power “Pp”. However, “t11” can besubstantially at the same time as “t10”. The waveform having a pulsetrain including four recording power Pw pulses is shown as an example ofrecording a mark of a specific length. The number of the recording powerPw pulses or the length of the pulse train varies depending upon data tobe recorded. The number of the recording power Pw pulses can be, forexample, from two to about ten.

FIG. 24B is a graph illustrating a waveform of a reflected light signalRF in the multiple-pulse recording method with the same time axis asthat of FIG. 24A. Between t0 to t11, the reflected light signal RFchanges in a very short time such that detection of the reflected lightsignal RF can be possible with a detection device having a relativelyfast operation speed. After t11, the waveform of a reflected lightsignal RF, which is circled and denoted as “g” in FIG. 24B, issubstantially the same as that of the single-pulse recording method.Accordingly, all of the embodiments described above can be practiced,not only with the single-pulse recording method, but also with themultiple-pulse recording method. In addition, regardless of thesingle-pulse recording method or the multiple-pulse recording method,the waveform shape of a reflected light signal RF is affected only by astate of a recorded-mark. FIG. 24C illustrates an exemplary “mark”formed by the multiple-pulse recording method.

FIG. 25 is a flowchart illustrating an exemplary operation ofcontrolling the recording-power of the optical information recordingapparatus 101 of FIG. 1, which is practiced with the multiple-pulserecording method. In the step S32, the laser diode 1 starts irradiatingthe recording medium 3 with recording-power Pw at time to of FIG. 24A,and forming of a recorded-mark M is started. During the steps S32 andS33, the laser diode control device 2 controls the laser diode 1 so asto form a recorded-mark such that a mark-state signal Vdtc to coincidethe control target Vtgt from the recording mark in step S37, utilizing apreviously obtained mark-state signal Vdtc.

In step S34, at time t2 of FIG. 24A, the laser diode control device 2switches the irradiation power of the laser diode 1 from therecording-power Pw to the bottom-power Pb. In Step S35, whether thenumber of operations corresponding to the number of recording pulses iscompleted is judged. When the number of operations corresponding to thenumber of recording pulses are completed at t10, the process proceeds tostep S36, where the formation of a recorded-mark M is completed, and theshape of the recorded-mark M is formed in a shape shown as “Mark M” inFIG. 24C . In step S36, at time t11, the light-receiving device 5receives the reflected light Pd from the recording medium 3 and convertsthe received light Pd into a received light signal RF. The receivedlight signal RF has the waveform as shown after t11 in FIG. 24B.

In step S37, the mark-state determining device 6 determines a state of arecorded-mark by using the received light signal RF and generates amark-state signal Vdtc as a feedback signal for a next recorded-markformation. The mark-state determining device 6 can use, in addition tothe received light signal RF, various information to detect the state ofa recorded-mark as described before. In Step S38, whether there is morerecording data to be recorded is judged.

FIG. 26 is a flowchart illustrating another exemplary operation ofcontrolling the recording-power. In this flowchart, the steps aresubstantially the same as those of FIG. 25 except step S36 b, step S37b. In the step S36 b, at each of times t2, t3, and t4, thelight-receiving device 5 receives the reflected light Pd from therecording medium 3 and converts each of the received light Pd into areceived light signal RF. The received light signal RF is obtained ateach of times t2, t3, and t4, as shown as “Vsbb” in FIG. 24B.

In step S37 b, the mark-state determining device 6 determines a state ofa recorded mark by using the received light signal RF and generates amark-state signal Vdtcb as a feedback signal for a next recorded-markformation. When each of the received light signal RF “Vsbb” obtained att2, t3, and t4 is close to the received light signal RF “Vsb” obtainedat t11, the feedback signal Vdtcb can be a value similar to the Vdtcgenerated in the step S37.

As described above, the present invention can be applied for recordingdata on a recording medium 3 having a recording layer that is recordableby a heat-mode reaction by the irradiation of the laser diode 1. In theheat-mode recording, a mark M is recorded by a change of opticalcharacteristics of the recording layer due to, for example, thermaldecomposition of the recording layer, vaporization of the recordinglayer, or distortion of the substrate of recording medium 3 by theirradiation. Generally, sensitivity of the heat-mode recording medium ishigh, and the all methods and apparatuses described above can be appliedfor recording on recording medium 3 having a heat sensitive recordinglayer. A certain kind of heat sensitive recording layer that includes,for example, such as cyanine compounds has characteristics that isdifferent from those of the described above. FIG. 27 is a graphillustrating waveforms of reflected light signal RF in the vicinity whena laser diode switched to output a pedestal power as a function of timefor comparison to a state of a recorded mark on a recording mediumhaving such a certain kind of heat sensitive recording layer. In FIG.27, “b” illustrates a waveform of the reflected light signal RF on amark recorded with an optimum irradiation power. As illustrated “b” ofFIG. 27, the reflected light signal RF is different from that of thedescribed above. The reflected light signal RF having a minimum value,shown as Vsb in FIG. 27, appears at a short time after the irradiationpower changes from the recording power Pw to the pedestal power Pp.

Each of “a” and “c” illustrates a waveform of the reflected light signalRF from a mark recorded with power smaller or larger than the optimumirradiation power. For example, when recording power Pw is too large,the minimum value Vsb of the reflected light signal RF shifts to Vsc.Likewise, a value Vsbt of the reflected light signal RF at time afterTa1 from t11 shifts to Vsct. A time tb after from t11, i.e., time whenthe value of the reflected light signal RF reaches a reference valueVref shifts to tc as well. Accordingly, the all methods and apparatusesdescribed above can be applied for recording on recording medium 3having such the certain kind of recording layer.

FIG. 28A, FIG. 28B, and FIG. 28C illustrate waveforms of irradiationlight power, a waveform of reflected light signal RF of a recorded-markon a recording medium having the certain kind of heat sensitiverecording layer, and a recorded-mark in the multiple-pulse recordingmethod in the heat mode recording.

As a material for heat-mode recording medium, for example, organiccoloring agents, such as, dyes of polymethylene compounds, cyaninecompounds, naphthalocyanine compounds, phthalocyanine compounds,squalirium compounds, pyrylium compounds, naphthoquinone compounds,anthraquinone compounds (indanthrene compounds), xanthene compounds,triphenylmethane compounds, azulene compounds, phenanthrene,triphenathiazine, and metal-complex compounds such as, azo compounds,can be utilized. These dyes can be dispersed in, compounded or stacked(multilayered) with other organic coloring agents, metals, and metalcompounds. As the metals and metal compounds, for example, indium,tellurium, bismuth, selenium, antimony, germanium, stannum (tin),aluminum, beryllium, tellurium dioxide, stannic oxide, arsenic, andcadmium can be utilized. For forming the recording layer, for example,such as a vacuum evaporation method, a spattering method, a chemicalvapour deposition method, and a solvent application method can beutilized. When the solvent application method is used, coloring agentsdescribed above are first dissolved in organic solvent, then thesolution is applied on a substrate of a recording medium by, forexample, a spray up method, a roller coating method, a dipping method,or a spin coating method.

The reaction velocity of the change of the optical characteristics of arecording layer while forming a recorded-mark on a recording mediumvaries depends on materials in the recording layer and thickness of therecording layer. When a certain kind of material is used, the opticalchange is not immediately completed when the irradiation light changesfrom the recording power Pw to the bottom power Pb or to the pedestalpower Pp, and as a result, forming of a recorded-mark M is continuedafter the recording power Pw is switched to the pedestal power Pp.Referring to FIG. 27, reference symbol tx is substantially equivalent toan interval between t11 to the time of completing the formation of arecorded-mark M. The amount of tx is also affected by a transient timefrom a time when the irradiation light has the recording power Pw to atime when the irradiation light has the pedestal power Pp. The amount oftx is also affected by the recording velocity and the difference of thematerial of the recording layer.

As described above, an optical information recording method and opticalinformation recording apparatus of the present invention are capable offorming an appropriate recorded-mark regardless of a recording medium ora recording method, by detecting a state of a recorded-mark andcontrolling the light source according to the determined state of therecorded-mark so as to output the recording power suitable for formingthe appropriate recorded-mark.

Obviously, numerous additional modifications and variations of thepresent invention are possible in light of the above teachings. It istherefore to be understood that within the scope of the appended claims,the present invention may be practiced otherwise than as specificallydescribed herein.

What is claimed as new and desired to be secured by Letters Patents of the United States is:
 1. A method of optically recording information on a recording medium, comprising: irradiating the recording medium with an irradiation light of a recording power to form a recorded-mark on the recording medium such that a reflection coefficient from an area of the recorded-mark is different than a reflection coefficient from an area of the recording medium where the recorded-mark is not formed, modulating the irradiation light according to the information for recording to form the recorded-mark on the recording medium by changing the power of the irradiation light between the recording power and a non-recording power; receiving a reflection light of the irradiation light reflected by the recording medium and producing a corresponding light signal; determining a state of the recorded-mark based upon the light signal produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power; controlling the recording power of the irradiation light according to the state of the recorded-mark; forming a plurality of test recording marks with a varied irradiation power on a predetermined area of the recording medium; receiving reflection light of the irradiation light reflected by the plurality of test recording marks and producing corresponding test light signals; storing in association each irradiation power and related test light signal; and determining an optimum pair of irradiation power and related test light signal as a control target value; said controlling step comprising, controlling the recording power of the irradiation light according to the state of the recorded-mark such that a value of the produced light signal becomes equivalent to the control target value.
 2. An apparatus for optically recording information on a recording medium by irradiating the recording medium with an irradiation light of a recording power to form a recorded-mark on the recording medium such that a reflection coefficient from an area of the recorded-mark is different than a reflection coefficient from an area of the recorded-medium where the recorded-mark is not formed, the apparatus comprising: a laser diode configured to irradiate the recording medium with light to form the recording mark by changing the power of the irradiation light between a recording power and a non-recording power; a light receiving device configured to receive a reflection light of the irradiation light reflected by the recording medium and to produce a corresponding light signal; a mark-state determining device configured to determine a state of the recorded-mark based upon the light signal produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power; and a laser diode control device configured to control the laser diode so as to modulate the recording power of the irradiation light according to the state of the recorded-mark, wherein the mark-state determining device comprises: a first sampling circuit configured to sample the light signal produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power, a second sampling circuit configured to sample the light signal produced by a non-recorded area of the recording medium; and a divider configured to divide the sampled light signal by the first sampling device relative to the light signal sampled by the second sampling device.
 3. An apparatus for optically recording information on a recording medium by irradiating the recording medium with an irradiation light of a recording power to form a recorded-mark on the recording medium such that a reflection coefficient from an area of the recorded-mark is different than a reflection coefficient from an area of the recorded-medium where the recorded-mark is not formed, the apparatus comprising: a laser diode configured to irradiate the recording medium with light to form the recording mark by changing the power of the irradiation light between a recording power and a non-recording power; a light receiving device configured to receive a reflection light of the irradiation light reflected by the recording medium and to produce a corresponding light signal; a mark-state determining device configured to determine a state of the recorded-mark based upon the light signal produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power; and a laser diode control device configured to control the laser diode so as to modulate the recording power of the irradiation light according to the state of the recorded-mark, wherein the mark-state determining device is configured to determine the state of the recorded-mark based upon a period of time from a time when power of the irradiation light changes to the non-recording power to a time when the produced light signal reaches a predetermined value, and wherein the mark-state determining device comprises: a comparator configured to compare the produced light signal with a predetermined reference value and to output a pulse; and a pulse width detector configured to detect the width of the output pulse.
 4. The apparatus according to claim 3, wherein the mark-state determining device comprises: a sampling circuit configured to sample the light signal produced by irradiation a non-recorded area of the recording medium; and, a reference value altering circuit configured to alter the reference value according to the light signal sampled by the sampling means such that the reference value has a value the same as the sampled light signal or a value that is a predetermined value smaller than the sampled light value.
 5. An apparatus for optically recording information on a recording medium, comprising: means for irradiating the recording medium with an irradiation light of a recording power to form a recorded-mark on the recording medium such that a reflection coefficient from an area of the recorded-mark is different than a reflection coefficient from an area of the recording medium where the recorded-mark is not formed; means for modulating the irradiation light according to the information for recording to form the recorded-mark on the recording medium by changing the power of the irradiation light between the recording power and a non-recording power; means for receiving a reflection light of the irradiation tight reflected by the recording medium and to produce a corresponding light signal; means for determining a state of the recorded-mark based upon the light signal which is produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power; and means for controlling the recording power of the irradiation light according to the state of the recorded-mark, wherein the means for determining comprises: first sampling means for sampling the light signal produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power; second sampling means for sampling the light signal produced by a non-recorded area of the recording medium; and normalizing means to normalize the light signal sampled by the first sampling means relative to the light signal sampled by the second sampling means.
 6. An apparatus for optically recording information on a recording medium, comprising: means for irradiating the recording medium with an irradiation light of a recording power to form a recorded-mark on the recording medium such that a reflection coefficient from an area of the recorded-mark is different than a reflection coefficient from an area of the recording medium where the recorded-mark is not formed; means for modulating the irradiation light according to the information for recording to form the recorded-mark on the recording medium by changing the power of the irradiation light between the recording power and a non-recording power; means for receiving a reflection light of the irradiation light reflected by the recording medium and to produce a corresponding light signal; means for determining a state of the recorded-mark based upon the light signal which is produced during a predetermined period of time immediately after power of the irradiation light changes to the non-recording power; and means for controlling the recording power of the irradiation light according to the state of the recorded-mark, wherein the determining means determines the state of the recorded-mark based upon a period of time from a time when power of the irradiation light changes to the non-recording power to a time when the produced light signal reaches a predetermined value, and wherein the determining means comprises: comparing means for comparing the produced light signal with a predetermined reference value and for outputting a pulse; and pulse width detecting means for detecting the width of the pulse.
 7. The apparatus according to claim 6, wherein the said determining means comprises: sampling means for sampling a light signal produced by irradiation of a non-recorded area of the recording medium; and, reference value altering means for altering the reference value according to the light signal sampled by the sampling means such that the reference value has a value the same as the sampled light signal or a value that is a predetermined value smaller than the sampled light value. 